Method for producing a fiber laser

ABSTRACT

To produce a fiber laser (106) a double-cladding active fiber (114) doped with Yb is predisposed to receive, near a first end (114a), a UV radiation suitable to write a first Bragg grating; during the writing process, a scanned pumping radiation is fed to the first end of the active fiber in order to excite an amplified stimulated emission between the first grating and the reflecting surface of a second end (114b) of the active fiber, previously cut and cleaned, and to consequently induce a laser emission from the active fiber; the optical power of the laser emission is measured and processed to obtain the laser efficiency; when a maximum value of the efficiency is reached, the writing process is stopped; similar steps are used to write a second grating near the second end (114b) of the active fiber.

CROSS REFERENCE TO RELATED APPLICATIONS

This application claims the benefit of European Application 99119319.4 filed Sep. 28, 1999 and U.S. Provisional Application No. 60/158,135 filed Oct. 8, 1999.

BACKGROUND OF THE INVENTION

1. Technical Field

The present invention relates to a method for producing a fiber laser.

2. Discussion

A fiber laser is an optical device comprising a doped optical fiber (active fiber) and a pump source adapted to provide a pump radiation to the doped optical fiber in order to excite the dopant. Rare earth elements used for doping typically include Erbium (Er), Neodymium (Nd), Ytterbium (Yb), Samarium (Sm), Thulium (TM) and Praseodymium (Pr). The particular rare earth element or elements used is determined in accordance with the wavelength of the laser emission and the wavelength of the pump light.

The excited dopant tends to generate, as a consequence of its de-excitation, a stimulated emission radiation. The fiber laser also includes reflecting elements suitable to confine the stimulated emission radiation inside the optical fiber and to allow, when predetermined amplification conditions are reached, the output of part of this radiation. The reflecting elements may be, for example, Bragg gratings written on opposite ends of the doped optical fiber. A Bragg grating includes an alternation of zones with high refraction index and zones of low refraction index, mutually spaced at a distance that establishes the reflection wavelength (Bragg wavelength).

Bragg gratings are typically written in the core of standard transmission fibers, i.e. fibers not doped for stimulated emission purposes, in order to define reflecting elements for the transmission signals. Prior to the writing process on a standard fiber, a photosensitizer is usually added to the core of the fiber in the region predisposed to host the grating. The writing process then includes the exposure of the photosensitized region to a UV radiation, which generates an interferential pattern in the said core region inducing a refraction index variation. The interferential pattern may be obtained by means of different techniques, of which the most used are the “phase mask” technique and the technique consisting in focusing on the said core region two interfering UV beams.

Real time information on the grating characteristics during writing may be obtained by feeding to one end of the optical fiber the radiation of a wide spectrum source (e.g. a white light lamp or a LED) and by detecting, by means of a spectrum analyzer, the reflection spectrum at the same end of the fiber or the transmission spectrum at the opposite end of the fiber. This setup offers information on the peak wavelength, the intensity and the shape of the grating, and these information can be used to control process parameters like the UV intensity, the writing duration and the grating length.

A further technique to get information related to the writing process comprises feeding to one end of the fiber a wavelength tuned laser radiation and detecting the reflection optical power (at the same fiber end) or the transmission optical power (at the opposite fiber end) by means of a power meter. This further technique is slower but allows a higher resolution with respect to the previous one. Then, the first technique (wide band radiation feeding) is preferably used for real time monitoring of the writing process, while the second (tuned laser radiation feeding) is preferably used for grating characterization at the end of the writing process.

An easy technique to realize a resonant cavity on an active fiber comprises joining the active fiber with two stretches of not doped optical fiber each including a Bragg grating having a Bragg wavelength at the predetermined laser wavelength. However, the unavoidable insertion losses at the fiber joining region induces a laser power reduction and undesired reflections inside the resonant cavity which degrade the laser performances.

A different solution consists in writing the Bragg gratings directly in the core of the active fiber. In this case, the high absorption of the active fiber at the wavelengths of the radiation fed to the fiber (i.e. the wavelengths used for the real time monitoring or for grating characterization) makes the above mentioned monitoring techniques impracticable.

Typically, before writing a grating on an active fiber an evaluation of the required exposure time is made by considering data previously collected on identical but not doped fibers. However, no information is available in this way on the effective grating reflectivity obtained at the end of the writing process and, consequently, on the effective laser efficiency.

The document of Mikael Svalgaard, “Ultraviolet light induced refractive index structures in germanosilica”, Ph. D. thesis, March 1997, Mikroelektronik Centret, Published by Mikroelektronik Centret, Technical University of Denmark, Building 345 east, DK-2800 Lyngby, Denmark, depicts in Chapter 4 a work addressed to investigate the frequency stability of Er-doped fiber lasers that incorporate Bragg fiber gratings as the end mirrors. Svalgaard indicates that the dynamics of forming Bragg gratings involves spectral shifts of the same order of magnitude as the grating bandwidth (typically a fraction of a nanometer) and that such small changes during UV writing critically affect the performance of the resulting fiber laser. A method is proposed for real time monitoring of the laser performance based on simultaneous UV grating fabrication and pumping of the Er doped fiber.

SUMMARY OF THE INVENTION

In the description of the experimental setup (paragraph 4.2), a 10 cm Er-doped fiber is considered, whose ends are spliced to standard telecommunication fiber. The (first) grating formation dynamics is monitored in transmission using a broadband 1550 nm LED source. The first grating is exposed until the transmittance at the Bragg wavelength is 0.028±0.001. During the writing of the second grating, Er-doped fiber is pumped by a 980 nm multimode diode laser through a 1530/980 nm wavelength-division multiplexing fiber coupler (WDM), and the laser output (near 1530 nm) is monitored on a spectrum analyzer. When the exposure time of the second grating approached that of the first, a maximum lasering power is reached. To prevent feedback optical isolators are used after both the diode and fiber lasers, and all fiber ends are angled. As reported in paragraph 4.3, to obtain robust single-frequency operation, the cavity must be very short. In the specific case, the cavity is 12.5±1 mm long. Furthermore, according to Svalgaard, it is critical that the second gratings Bragg wavelength matches that of the first for lasering to occur.

The Applicant has observed that the fiber laser considered in the above document is a single-longitudinal-mode wavelength stabilized doped fiber laser, which includes an active fiber having a relatively low absorption at the Bragg wavelength, mainly due to the fact that the fiber is very short. This feature allows using a standard technique (feeding a wide band radiation to the fiber and detecting the related fiber output spectrum) for monitoring the characteristics of the first grating during the writing process.

The Applicant has noticed that, if a fiber laser has to be realized which includes an active fiber having a high absorption at the Bragg wavelength, the above method is no more suitable.

For the aim of the present invention, with “high absorption” it is intended an absorption of at least 15 dB in a range of about ±10 nm centered at the Bragg wavelength. The absorption of the fiber depends mainly on its geometry, on its length and on the dopant concentration.

The Applicant has in particular noticed that the first grating writing monitoring by means of a LED source or another wide band source would not be possible in case of a high absorption fiber, due to the excessive signal loss inside the fiber which would avoid correct spectrum detection.

Fiber lasers including a high absorption active fiber may be used, for example, as pump sources for optical amplifiers in optical transmission systems. For this kind of application, it is nor required to have a single-mode stabilized laser radiation and the active fiber is preferably designed so as to maximize the pump absorption. Then, the active fiber is preferably a relatively long and heavily doped fiber. It is further known that, in order to achieve a very high pump absorption, a fiber laser may advantageously include a double-cladding active fiber, i.e. an active fiber having a core for laser emission, an inner cladding larger than the core to receive the pump radiation and an outer cladding. The pump radiation is progressively transferred from the inner cladding to the core for dopant excitation. A fiber laser including a double-cladding active fiber is known, for example, from U.S. Pat. No. 5,530,709 in the name of SDL, Inc.

The Applicant has noticed that additional difficulties in the grating writing monitoring would arise if the considered active fiber is a double-cladding fiber. In fact, in this case the light of a wide band source will propagate mainly inside the inner cladding (having a geometrical section area much greater than the core) and the detected spectrum will then provide no indication on the grating written into the core. If the active fiber is a double-cladding fiber, the above condition on the absorption of the fiber is more pressing, and absorption values much lower than 15 dB (in a range of about ±10 nm centered at the Bragg wavelength) are sufficient to avoid the correct use of the known techniques.

The Applicant has found that a method for realizing a fiber laser including a high absorption active fiber comprises defining a reflecting surface associated to the active fiber and, during the first grating writing, pumping the active fiber in order to cause an amplified spontaneous emission between the first grating and the reflecting surface, and a consequent laser emission. This laser emission is detected and processed so as to allow a control of the laser performances during the writing process. The method then includes writing the second grating in a similar manner, where the resonant cavity is now defined between the first and the second grating.

The Applicant has found that, during the grating writing process, by repeatedly scanning the pump radiation fed to the active fiber between a minimum and a maximum value and by adeguately processing the output power from the active fiber, it is possible to derive real time values of the lasers efficiency and threshold power, which can be advantageously used to control the grating reflectivity in order to reach optimized laser performances.

According to a first aspect, the present invention relates to a method for producing a fiber laser, including writing a first grating having a first reflection wavelength band in an active fiber and includes the following steps:

defining a reflecting surface associated to the active fiber, before the step of writing said first grating, said reflecting surface having a second reflection wavelength band wider than the first reflection wavelength band;

optically pumping the active fiber, during the step of writing the first grating, in order to excite an amplified stimulated emission between the first grating and the reflecting surface and to consequently induce a laser emission from the active fiber;

measuring, during the step of writing the first grating, the optical power of the laser emission;

controlling the step of writing the first grating according to the measured optical power.

Preferably, the method includes writing in the active fiber, subsequently to the first grating, a second grating suitable to define, together with the first grating, a resonant cavity for said fiber laser.

The method preferably includes, during the step of writing the first grating, scanning the power of the pump radiation in a predetermined power range.

Preferably, the step of scanning is repeated with a predetermined scanning period and the step of measuring the optical power includes obtaining a predetermined number of optical power values during the predetermined scanning period.

The step of obtaining a predetermined number of optical power values preferably includes calculating, to obtain each of said optical power values, the average value of the optical power measured in a predetermined measuring period.

The method preferably includes the step of processing said optical power values in order to obtain a current value of the laser efficiency.

The step of processing preferably comprises finding a fitting line for a predetermined number of points on a laser gain characteristic corresponding to said optical power values, and evaluating the slope of said line.

The step of controlling the step of writing preferably includes checking if said current value of the laser efficiency has reached a limit value and, if said limit value has been reached, stopping the step of writing the first grating.

The step of checking preferably includes comparing said current value of the laser efficiency, related to a last scanning period, with a preceding value of the laser efficiency, related to a preceding scanning period.

The method preferably includes evaluating, according to said limit value, the reflectivity of said first grating.

The step of defining a reflecting surface preferably includes cutting and cleaning one end of the active fiber in order to define the reflecting surface at the interface glass/air.

The active fiber preferably has an absorption of at least 15 dB in a range of about ±10 nm centered at a wavelength corresponding to a maximum reflection wavelength of said first grating.

The active fiber preferably includes a double-cladding active fiber.

The method preferably includes the following steps:

optically pumping the active fiber, during the step of writing the second grating, in order to excite an amplified stimulated emission between said first and second gratings and consequently induce a laser emission from the active fiber;

measuring, during the step of writing the second grating, the optical power of the laser emission;

controlling the step of writing the second grating according to the measured optical power.

The method preferably includes, during the step of writing the second grating, scanning the power of the pump radiation in a predetermined power range.

The step of scanning is preferably repeated with a predetermined scanning period and the step of measuring the optical power preferably includes obtaining a predetermined number of optical power values during the predetermined scanning period.

The step of obtaining a predetermined number of optical power values preferably includes calculating, to obtain each of said optical power values, the average value of the optical power measured in a predetermined measuring period.

The method preferably includes the step of processing said optical power values in order to obtain a current value of the laser efficiency.

The step of processing preferably comprises obtaining from said optical power values a current value of the laser threshold power.

The step of controlling the step of writing preferably includes checking if said current value of the laser efficiency has reached a maximum value and, if said maximum value has been reached, stopping the step of writing the second grating.

The step of controlling the step of writing preferably includes stopping the step of writing the second grating when a predetermined relation between said current values of the laser efficiency and the threshold power has been reached.

The method preferably includes evaluating, according to said maximum value, the reflectivity of said second grating.

The method preferably includes, before the step of writing the second grating, defining a zone of negligible reflectivity in place of said reflecting surface.

Preferably, the second grating has a third reflection wavelength band and the ratio between the third and the first reflection wavelength bands is between 1,5 and 3.

According to a further aspect, the present invention relates to a fiber laser, including an active fiber, a first grating written in a first portion of the active fiber and having a first reflection wavelength band, and a second grating written in a second portion of the active fiber and having a second reflection wavelength band, the first and the secong grating defining a resonant cavity for the fiber laser, wherein in that the ratio between the widths of said first and said second reflection wavelength bands is between 1.5 and 3.

The active fiber preferably includes a double-cladding active fiber.

The active fiber preferably has an absorption of at least 15 dB in a range of about ±10 nm centered at a wavelength corresponding to the center of said reflection wavelength band.

BRIEF DESCRIPTION OF THE DRAWINGS

The foregoing general description and the following detailed description are exemplary and explanatory only and are not restrictive of the invention as claimed.

The following description, as well as the practice of the invention, set forth and suggest additional advantages and purposes of this invention.

The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate embodiments of the invention, and together with the description, explain the advantages and principles of the invention.

FIG. 1 is a block diagram of an optical transmission system consistent with the present invention;

FIG. 2 is a qualitative graph of the spectral gain characteristic of the optical transmission system of FIG. 1, with a designation of the signal transmission bands (BB, RB1 and RB2);

FIG. 3 is a more detailed diagram of the multiplexing section of the optical transmission system in FIG. 1;

FIG. 4 is a more detailed diagram of the transmitter power amplifier section of the optical transmission system in FIG. 1;

FIG. 5 is a graph of a filter performance shape of a de-emphasis filter for the optical transmission system of FIG. 1;

FIG. 6 is a detailed diagram of an intermediate station of the optical transmission system of FIG. 1;

FIG. 7 is a detailed diagram of a receiver pre-amplifier section of the optical transmission system of FIG. 1;

FIG. 8 is a detailed diagram of a multiplexing section of the optical transmission system of FIG. 1;

FIG. 9 is a schematic representation of an optical amplifying unit according to the present invention;

FIG. 10 is a schematic representation of a pump source included in the optical amplifying unit of FIG. 9;

FIGS. 11a and 11 b are schematic representations of a double-cladding fiber used for the pump source of FIG. 10 and of the multi-mode pumping operation of a double cladding fiber;

FIGS. 12 shows a grating writing assembly used to write gratings in the double-cladding fiber of the pump source of FIG. 10;

FIG. 13 shows the response curve of a fiber laser used for experimental measurements;

FIGS. 14 and 15 illustrate experimental results obtained with an amplifying unit according to the invention;

FIGS. 16 and 17 are flux diagrams of a method for writing gratings in an active fiber used for the pump source of FIG. 10;

FIGS. 18a and 18 b show schematically the variation of a predetermined parameter during the grating writing process according to the method of FIGS. 17a and 17 b;

FIGS. 19-21 show the simulated performances of a fiber laser used for the pump source of FIG. 10.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Referring to FIG. 1, an optical transmission system 1 includes a first terminal site 10, a second terminal site 20, an optical fiber line 30 connecting the two terminal sites 10, 20, and at least one line site 40 interposed between the terminal sites 10 and 20 along the optical fiber line 30.

For simplicity, the optical transmission system 1 hereinafter described is unidirectional, that is signals travel from a terminal site to the other (in the present case from the first terminal site to the second terminal site), but any consideration that follow is to be considered valid also for bidirectional systems, in which signals travel in both directions. Further, although the optical transmission system 1 is adapted to transmit up to one-hundred-twenty-eight (128) channels, from the hereinafter description it will be obvious that the number of channels is not a limiting feature for the scope and the spirit of the invention, and less or more than one-hundred-twenty-eight (128) channels can be used depending on the needs and requirements of the particular optical transmission system.

The first terminal site 10 preferably includes a multiplexing section (MUX) 11 adapted to receive a plurality of input channels 16, and a transmitter power amplifier section (TPA) 12. The second terminal site 20 preferably includes a receiver pre-amplifier (RPA) section 14 and a demultiplexing section (DMUX) 15 adapted to output a plurality of output channels 17.

Multiplexing section 11, hereinafter described with reference to FIG. 3, multiplexes or groups input channels 16 preferably into three sub-bands, referred to as blue-band BB, first red-band RB1 and second red-band RB2, although multiplexing section 11 could alternatively group input channels 16 into a number of sub-bands greater or less than three.

The three sub-bands BB, RB1 and RB2 are then received, as separate sub-bands or as a combined wide-band, in succession by TPA section 12, at least one line site 40 and second terminal site 20. Sections of optical fiber line 30 adjoin the at least one line site 40 with TPA section 12, RPA section 14, and possibly with others line sites 40 (not shown). TPA section 12, that will be later described with reference to FIG. 4, receives the separate sub-bands BB, RB1 and RB2 from multiplexing section 11, amplifies and optimizes them, and then combines them into a single wide-band SWB for transmission on a first section of optical fiber line 30. Line site 40, that will be later described with reference to FIG. 6, receives the single wide-band SWB, re-divides the single wide-band SWB into the three sub-bands BB, RB1 and RB2, eventually adds and drops signals in each sub-band BB, RB1 and RB2, amplifies and optimizes the three sub-bands BB, RB1 and RB2 and then recombines them into the single wide-band SWB. For the adding and dropping operations, line site 40 may be provided with Optical Add/Drop Multiplexers (OADM) of a known type or, for example, of the type described in EP patent application No. 98110594.3 in the name of the Applicant.

A second section of optical fiber line 30 couples the output of the line site 40 to either another line site 40 (not shown) or to RPA section 14 of second terminal site 20. RPA section 14, that will be later described with reference to FIG. 7, also amplifies and optimizes the single wide-band SWB and may split the single wide-band SWB into the three sub-bands BB, RB1 and RB2 before outputting them.

Demultiplexing section 15, that will be later described with reference to FIG. 8, receives the three sub-bands BB, RB1 and RB2 from RPA section 14 and splits the three sub-bands BB, RB1 and RB2 into the individual wavelengths of output channels 17. The number of input channels 16 and output channels 17 may be unequal, owing to the fact that some channels can be dropped and/or added in line site (or line sites) 40.

According to the above, for each sub-band BB, RB1 and RB2 an optical link is defined between the corresponding input of TPA section 12 and the corresponding. output of RPA section 14.

FIG. 2 is a qualitative graph of the spectral emission ranges of the amplifiers used in the optical transmission system 1 and approximately corresponding to the different gain for channels of signals traveling through the fiber link and the different allocation of the three sub-bands BB, RB1 and RB2. In particular, the first sub-band BB preferably covers the range between 1529 nm and 1535 nm, corresponds to a first amplification wavelength range of erbium-doped fiber amplifiers and allocates up to sixteen (16) channels; the second sub-band RB1 falls between 1541 nm and 1561 nm, corresponds to a second amplification wavelength range of erbium-doped fiber amplifiers and allocates up to forty-eight (48) channels; and the third sub-band RB2 covers the range between 1575 nm and 1602 nm, corresponds, according to the invention, to an amplification wavelength range of erbium/ytterbium-doped fiber amplifiers and allocates up to sixty-four (64) channels. The gain spectral graph of the erbium/ytterbium-doped fiber amplifiers is such that, although the 1575-1502 nm range offers the best performances in terms of amplification, channels can be advantageously allocated down to 1565 nm and up to 1620 nm.

Adjacent channels, in the proposed one-hundred-twenty-eight (128) channel system, have preferably a 50 GHz constant spacing. Alternatively, a different constant spacing may be used, or the frequency spacing may be unequal to alleviate the known four-wave-mixing phenomenon.

In the erbium amplification band, the RB1 and RB2 bands have a fairly flat gain characteristic, while the BB band includes a substantial hump in the gain response. As explained below, to make use of the erbium-doped fiber spectral emission range in the BB band, optical transmission system 1 uses equalizing means to flatten the gain characteristic in that range. As a result, by dividing the erbium-doped fiber spectral emission range of 1529-1502 nm into three sub-ranges that respectively include the BB band, RB1 band and RB2 band, optical transmission system 1 can effectively use most of the erbium-doped fiber spectral emission range and provide for dense WDM.

The following provides a more detailed description of the various modules of the present invention depicted in FIG. 1.

FIG. 3 shows a more detailed diagram of the first terminal site 10. The first terminal site 10 includes, in addition to the multiplexing section 11 and the TPA section 12 (not shown in FIG. 3), an optical line terminal section (OLTE) 41 and a wavelength converter section (WCS) 42.

OLTE 41, which may correspond to standard line terminating equipment for use in a standard system, e.g. a SONET, ATM, IP or SDH system, includes transmit/receive (TX/RX) units (not shown) in a quantity that equals the number of channels in WDM systems 10. In a preferred embodiment, OLTE 41 has one-hundred-twenty-eight (128) TX/RX units. In multiplexing section 11, OLTE 41 transmits a plurality of signals at a generic wavelength. As shown in FIG. 3, in a preferred embodiment OLTE 41 outputs a first group of sixteen (16) channels, a second group of forty-eight (48) channels and a third group of sixty-four (64) channels. However, as indicated above, the number of channels may vary depending on the needs and requirements of the particular optical transmission system.

As readily understood to one of ordinary skill in the art, OLTE 41 may comprise a collection of smaller separate OLTEs, such as three, that feed information frequencies to WCS 42. Accordingly, WCS 42 includes one-hundred-twenty-eight (128) wavelength converter modules WCM1-WCM128.

Units WCM1-WCM16 each receive a respective one of the first group of signals emitted from OLTE 41, units WCM17-WCM64 each receive one of the second group of signals emitted from OLTE 41 and units WCM65-WCM128 each receive one of the third group of signals emitted from OLTE 41. Each unit is able to convert a signal from a generic wavelength to a selected wavelength and re-transmit the signal. The units may receive and re-transmit a signal in a standard format, such as OC-48 or STM-16, but the preferred operation of WCM1-128 is transparent to the particular data format employed.

Each WCM1-128 preferably comprises a module having a photodiode (not shown) for receiving an optical signal from OLTE 41 and converting it to an electrical signal, a laser or optical source (not shown) for generating a fixed carrier wavelength, and an electro-optic modulator such as a Mach-Zehnder modulator (not shown) for externally modulating the fixed carrier wavelength with the electrical signal. Alternatively, each WCM1-128 may comprise a photodiode (not shown) together with a laser diode (not shown) that is directly modulated with the electrical signal to convert the received wavelength to the carrier wavelength of the laser diode. As a further alternative, each WCM1-128 comprises a module having a high sensitivity receiver (e.g., according to SDH or SONET standards) for receiving an optical signal, e.g., via a wavelength demultiplexer, from a trunk fiber line end and converting it to an electrical signal, and a direct modulation or external modulation laser source. By the latter alternative, regeneration of signals from the output of a trunk fiber line and transmission in the inventive optical communication system is made possible, which allows extending the total link length.

Although FIG. 3 shows that the signals are provided and generated by the combination of OLTE 41 and WCM1-WCM128, the signals can also be directly provided and generated by a source without limitation to their origin.

The multiplexing section 11 includes three wavelength multiplexers (WM) 43, 44 and 45. For the preferred one-hundred-twenty-eight (128) channels system, each selected wavelength signal output from units WCM1-WCM16 is received by WM 43, each selected wavelength signal output from WCM17-WCM64 is received by WM 44 and each selected wavelength signal output from WCM65-WCM128 is received by WM 45. WM 43, WM 44 and WM 45 combine the received signals of the three bands BB, RB1 and RB2 into three respective wavelength division multiplexed signals. As shown in FIG. 3, WM 43 is a sixteen (16) channels wavelength multiplexer, such as a conventional 1×16 planar optical splitter, WM 44 is a forty-eight (48) channels wavelength multiplexer, such as a conventional 1×64 planar optical splitter with sixteen (16) unused ports and WM 45 is a sixty-four (64) channels wavelength multiplexer, such as a conventional 1×64 planar optical splitter. Each wavelength multiplexer may include a second port (e.g. 2×16 and 2×64 splitters) for providing optical transmission system 1 with an optical monitoring channel (not shown). As well, WM 43, 44 and 45 may have more inputs than is used by the system to provide space for system growth. A wavelength multiplexer using passive silica-on-silicon (SiO₂—Si) or silica-on-silica (SiO₂—SiO₂) technology, for instance, can be made by one of ordinary skill in the art. Other technologies can also be used for WMs, e.g., for reducing insertion losses. Examples are AWG (Arrayed Waveguide Gratings), cascaded Mach-Zehnder, fiber gratings, and interferential filters.

With reference to FIG. 4, the BB, RB1 and RB2 band output from multiplexing section 11 are received by TPA section 12. The BB, RB1 and RB2 band signals may be provided to TPA section 12 from a source other than the OLTE 41, WCS 42, and WM 43, 44 and 45 configuration depicted in FIG. 3. For example, the BB, RB1 and RB2 band signals may be generated and directly supplied to TPA section 12 by a customer without departing from the intent of the present invention described in more detail below.

TPA section 12 includes three amplifier sections 51, 52, 53, each for a respective band BB, RB1 and RB2, a coupling filter 54 and an equalizing filter 61. Amplifier sections 51, 52 are preferably erbium-doped two-stages fiber amplifiers (although other rare-earth-doped fiber amplifiers may be used), while amplifier section 53 is, according to the invention, an erbium/ytterbium-doped (ErJ>b) fiber amplifier that will be described in details with reference to FIG. 9.

The outputs of amplifiers 51, 52 and 53 are received by filter 54, which combines the BB, RB1 and RB2 bands into a single wide-band (SWB).

Each of the amplifiers 51 and 52 is pumped by one or two laser diodes to provide optical gain to the signals it amplifies. The characteristics of each amplifier, including its length and pump wavelength, are selected to optimize the performance of that amplifier for the particular subband that it amplifies. For example, the first stage (pre-amplifier) of amplifier sections 51 and 52 may be pumped with a laser diode (not shown) operating at 980 nm to amplify the BB band and the RB1 band, respectively, in a linear or in a saturated regime. Appropriate laser diodes are available from the Applicant. The laser diodes may be coupled to the optical path of the pre-amplifiers using 980/1550 WDM couplers (not shown) commonly available on the market, for example model SWDM0915SPR from E-TEK DYNAMICS, INC., 1885 Lundy Ave., San Jose, Calif. (USA). The 980 nm laser diode provides a low noise figure for the amplifiers compared with other possible pump wavelengths.

The second stage of each amplifier section 51-53 preferably operates in a saturated condition. The second stage of amplifier section 51 is preferably erbium-doped and amplifies the BB band with another 980 nm pump (not shown) coupled to the optical path of the BB band using a WDM coupler (not shown) described above. The 980 nm pump provides better gain behavior and noise figure for signals in the low band region that covers 1529-35 nm. The second stage of amplifier section 52 is preferably erbium-doped and amplifies the RB1 band with a laser diode pump source operating at 1480 nm. Such a laser diode is available on the market, such as model FOL1402PAX-1 supplied by JDS FITEL, INC., 570 Heston Drive, Nepean, Ontario (Calif.). The 1480 nm pump provides better saturated conversion efficiency behavior, which is exploited in the RB1 band for the greater number of channels in the region that covers 1542-61 nm. Alternatively, a higher power 980 nm pump laser or multiplexed pump sources in the 980 nm wavelength region may be used. Section 53 will be hereunder described in details with reference to FIGS. 9.

Filter 61 is positioned within the RB1 band amplifier chain for helping to equalize signal levels and SNRs at the system output across the RB1 band. In particular, filter 61 comprises a de-emphasis filter that attenuates the wavelength regions of the high amplification within the RBI band. The de-emphasis filter, if used, may employ long period Bragg grating technology, split-beam Fourier filter, etc. As an example, the de-emphasis filter may have an operating wavelength range of 1541-1561 nm and have wavelengths of peak transmission at 1541-1542 nm and 1559-1560 nm, with a lower, relatively constant transmission for the wavelengths between these peaks. FIG. 5 illustrates the filter shape or relative attenuation performance of a preferred de-emphasis filter 61. The graph of FIG. 5 shows that the de-emphasis filter 61 has regions of peak transmission at around 1542 nm and 1560 nm, and a region of relatively constant or flat attenuation between about 1546 nm and 1556 nm. The de-emphasis filter 61 for erbium-doped fiber amplifiers need only add an attenuation of about 3-4 dB at wavelengths between the peaks to help flatten the gain response across the high band. The de-emphasis filter 61 may have an attenuation characteristic different from that depicted in FIG. 5 depending on the gain-flattening requirements of the actual system employed, such as the dopant used in the fiber amplifiers or the wavelength of the pump source for those amplifiers.

Alternatively, the de-emphasis filter 61 may be omitted and the de-emphasis operation may be obtained in the multiplexing section 11 of the first terminal site 10 by means of calibrated attenuation.

After passing through the amplifiers of TPA 12, the amplified BB, RB1 and RB2 bands output from amplifier sections 51, 52 and 53, respectively, are received by filter 54. Filter 54 is a band combining filter and may, for example, include two cascaded interferential three port filter (not shown), the first coupling the BB band with the RB1 band and the second coupling the BB/RB1 bands provided by the first filter with the RB2 band.

An optical monitor (not shown) and insertion for a service line, at a wavelength different from the communication channels, e.g. at 1480 nm, through a WDM 1480/1550 interferential filter (not shown) may also be added at the common port. The optical monitor detects optical signals to ensure that there is no break in optical transmission system 1. The service line insertion provides access for a line service module, which can manage through an optical supervisory channel the telemetry of alarms, surveillance, monitoring of performance and data, controls and housekeeping alarms, and voice frequency orderwire.

The single wide-band output from filter 54 of TPA section 12 passes through a length of transmission fiber (not shown) of optical fiber line 30 such as 100 kilometers, which attenuates the signals within the single wide-band SWB. Consequently, line site 40 receives and amplifies the signals within the single wide-band SWB. As shown in FIG. 6, line site 40 includes several amplifiers (AMP) 64-69, three filters 70-72, an equalizing filter (EQ) 74 and three OADM stages 75-77.

Filter 70 receives the single wide-band SWB and separates the RB2 band from the BB and the RB1 bands. Amplifier 64 receives and amplifies the BB and the RB1 bands, whereas filter 71 receives the output from amplifier 64 and separates the BB band and the RB1 band. The BB band is equalized by equalizing filter 74, received by the first OADM stage 75 where predetermined signals are dropped and/or added, and further amplified by amplifier 65. The RB1 band, which has already passed through de-emphasis filter 61 in TPA 12, is first amplified by amplifiers 66, then received by the second OADM stage 76 where predetermined signals are dropped and/or added, and further amplified by amplifier 67. The RB2 band is first amplified by amplifier 68, then received by the third OADM stage 77 where predetermined signals are dropped and/or added, and further amplified by amplifier 69. The amplified BB, RB1 and RB2 bands are then recombined into the single wide-band SWB by filter 72.

Amplifier 64, which receives the single wide-band SWB, preferably comprises a single optical fiber amplifier that is operated in a linear regime. That is, amplifier 64 is operated in a condition where its output power is dependent on its input power. Depending on the actual implementation, amplifier 64 may alternatively be a single-stage or a multi-stage amplifier. By operating it in a linear condition, amplifier 64 helps to ensure relative power independence between the BB and RB1 band channels. In other words, with amplifier 64 operating in a linear condition, the output power (and signal-to-noise ratio) of individual channels in the one of the two sub-bands BB, RB1 does not vary significantly if channels in the other sub-band RB1, BB are added or removed. To obtain robustness with respect to the presence of some or all of the channels in a dense WDM system, first stage amplifier (such as amplifier 64 and amplifier 68) must be operated, in a line site 40, in an unsaturated regime, before extracting a portion of the channels for separate equalization and amplification. In a preferred embodiment, amplifiers 64 and 68 are erbium-doped fiber amplifiers, pumped in a co-propagating direction with a laser diode (not shown) operating at 980 nm pump to obtain a noise figure preferably less than 5.5 dB for each band.

Filter 71 may comprise, for example, a three-port device, preferably an interferential filter, having a drop port that feeds the BB band into equalizing filter 74 and a reflection port that feeds the RB1 band into amplifier 66.

Amplifier 66 is preferably a single erbium-doped fiber amplifier that is operated in saturation, such that its output power is substantially independent from its input power. In this way, amplifier 66 serves to add a power boost to the channels in the RB1 band compared with the channels in the BB band. Due to the greater number of channels in the RB1 band compared with the BB band in the preferred embodiment, i.e. forty-eight (48) channels as opposed to sixteen (16), the RB1 band channels typically will have had a lower gain when passing through amplifier 64. As a result, amplifier 66 helps to balance the power for the channels in the RB1 band compared with the BB band. Of course, for other arrangements of channels between the BB and the RB1 bands, amplifier 66 may not be required or may alternatively be required on the BB band side of line site 40.

With respect to the RB1 band of channels, amplifiers 64 and 66 may be viewed together as a two-stage amplifier with the first stage operated in a linear mode and the second stage operated in saturation. To help stabilize the output power between channels in the RB1 band, amplifier 64 and 66 are preferably pumped with the same laser diode pump source. In this manner, as described in EP 695049, the residual pump power from amplifier 64 is provided to amplifier 66. Specifically, line site 40 includes a WDM coupler positioned between amplifier 64 and filter 71 that extracts 980 nm pump light that remains at the output of amplifier 64. This WDM coupler may be, for example, model number SWDMCPR3PS110 supplied by E-TEK DYNAMICS, INC., 1885 Lundy Ave., San Jose, Calif. (USA). The output from this WDM coupler feeds into a second WDM coupler of the same type and positioned in the optical path after amplifier 66. The two couplers are joined by an optical fiber 78 that transmits the residual 980 nm pump signal with relatively low loss. The second WDM coupler passes the residual 980 nm pump power into amplifier 66 in a counter-propagating direction.

From amplifier 66, RB1 band signals are conveyed to OADM stage 76 of a known type or of the type described in EP patent application No. 98110594.3 in the name of the Applicant. From OADM stage 76, RB1 band signals are fed to amplifier 67. For the preferred erbium-doped fiber amplifier, amplifier 67 has a pump wavelength of, for example, 1480 nm from a laser diode source (not shown) having a pump power in excess of the laser (not shown) that drives amplifiers 64 and 66. The 1480 nm wavelength provides good conversion efficiency for high output power output compared with other pump wavelengths for erbium-doped fibers. Alternatively, a high power 980 nm pump source or a group of multiplexed pump sources, such as one at 975 nm and another at 986 nm, or two polarization multiplexed pump sources at 980 nm, could be used to drive amplifier 67. Amplifier 67 preferably operates in saturation to provide the power boost to the signals within the RB1 band, and if desired, may comprise a multi-stage amplifier.

After passing through amplifier 64 and filter 71, the BB band enters equalizing filter 74. As discussed above, the gain characteristic for the erbium-doped fiber spectral emission range has a peak or hump in the BB band region, but remains fairly flat in the RB1 band region. As a result, when the BB band or the single wide-band SWB (which includes the BB band) is amplified by an erbium-doped fiber amplifier, the channels in the BB band region are amplified unequally. Also, as discussed above, when equalizing means have been applied to overcome this problem of unequal amplification, the equalizing has been applied across the entire spectrum of channels, resulting in continued gain disparities. However, by splitting the spectrum of channels into a BB band and a RB1 band, equalization in the reduced operating area of the BB band can provide proper flattening of the gain characteristic for the channels of the BB band.

In a preferred embodiment, the equalizing filter 74 comprises a two-port device based on long period chirped Bragg grating technology that gives selected attenuation at different wavelengths. For instance, equalizing filter 74 for the BB band may have an operating wavelength range of 1529 nm to 1536 nm, with a wavelength at the bottom of the valley at between 1530.3 nm and 1530.7 nm. Equalizing filter 74 need not be used alone and may be combined in cascade with other filters (not shown) to provide an optimal filter shape, and thus, gain equalization for the particular amplifiers used in the WDM system 1. Equalizing filter 74 may be manufactured by one skilled in the art, or may be obtained from numerous suppliers in the field. It is to be understood that the particular structure used for the equalizing filter 74 is within the realm of the skilled artisan and may include, for instance, a specialized Bragg grating like a long period grating, an interferential filter, or Mach-Zehnder type optical filters.

From equalizing filter 74, BB band signals are conveyed to OADM stage 75, which is, for example, of the same type of OADM stage 76, and then to amplifier 65. With the preferred erbium-doped fiber amplifier, amplifier 65 has a pump wavelength of 980 nm, provided by a laser diode source (not shown) and coupled via a WDM coupler (not shown) to the optical path for pumping the amplifier 65 in a counter-propagating direction. Since the channels in the BB band pass through both amplifier 64 and amplifier 65, equalizing filter 74 may compensate for the gain disparities caused by both amplifiers. Thus, the decibel drop for equalizing filter 74 should be determined according to the overall amplification and line power requirements for the BB band. The amplifier 65 preferably operates in saturation to provide a power boost to the signals in the BB band, and may comprise a multi-stage amplifier if desired.

The RB2 band is received from fiber amplifier 68, which is, preferably, an erbium doped fiber amplifier pumped with a 980 nm or a 1480 nm pump light, depending on the system requirements. From amplifier 68, RB2 band channels are conveyed to OADM stage 77, which is, for example, of the same type of OADM stages 75 and 76, and then fed to amplifier 69. Amplifier 69 is, according to the invention, an erbium/ytterbium co-doped amplifier adapted to amplify the RB2 band and will be described in details with reference to FIG. 10.

After passing through amplifiers 65, 67 and 69 respectively, the amplified BB, RB1 and RB2 bands are then recombined by filter 72 into the single wide-band SWB. Like filter 54 of FIG. 4, filter 72 may, for example, include two cascaded interferential three port filter (not shown), the first coupling the BB with the RB1 bands and the second coupling the BB and RB1 bands provided by the first filter with the RB2 band.

Like TPA section 12, line site 40 may also include an optical monitor and a service line insertion and extraction (not shown) through, e.g., a WDM 1480/1550 interferential filter (not shown). One or more of these elements may be included at any of the interconnection points of line site 40.

Besides amplifiers 64-69, filters 70-72 and 74, and OADM stages 75-77, line site 40 may also include a dispersion compensating module (DCM) (not shown) for compensating for chromatic dispersion that may arise during transmission of the signals along the long-distance communication link. The DCM (not shown) is preferably comprised of subunits coupled upstream one or more of amplifiers 65, 67, 69 for compensating the dispersion of channels in one or more than one of the BB, RB1, RB2 bands, and may also have several forms. For example, the DCM may have an optical circulator with a first port connected to receive the channels in the three bands BB, RB1 and RB2. A chirped Bragg grating may be attached to a second port of the circulator. The channels will exit the second port and be reflected in the chirped Bragg grating to compensate for chromatic dispersion. The dispersion compensated signals will then exit a next port of the circulator for continued transmission in the WDM system. Other devices besides the chirped Bragg grating, such as a length of dispersion compensating fiber, may be used for compensating the chromatic dispersion. The design and use of the DCM section are not limiting the present invention and the DCM section may be employed or omitted in the WDM system 1 depending on overall requirements for system implementation.

After the line site 40, the combined single wide-band SWB signal passes through a length of long-distance optical transmission fiber of optical fiber line 30. If the distance between the first and the second terminal site 10, 20 is sufficiently long to cause attenuation of the optical signals, i.e. 100 kilometers or more, one or more additional line sites 40 providing amplification may be used. In a practical arrangement, five spans of long-distance transmission fiber are used (each having a power loss of 0.22 dB/km and a length such as to provide a total span loss of approximately 25 dB), separated by four amplifying line site 40.

Following the final span of transmission fiber, RPA section 14 receives the single wide-band SWB from last line site 40 and prepares the signals of the single wide-band SWB for reception and detection at the end of the communication link. As shown in FIG. 7, RPA section 14 may include amplifiers (AMP) 81-85, filters 86 and 87, an equalizing filter 88 and, if necessary, three router modules 91-93.

Filter 86 receives the single wide-band SWB and separates the RB2 band from the BB and RB1 bands. Amplifier 81 is preferably doped with erbium and amplifies the BB and RB1 bands to help improve the signal-to-noise ratio for the channels in the BB and RB1 bands. Amplifier 81 is pumped, for example, with a 980 nm pump or with a pump at some other wavelength to provide a low noise figure for the amplifier. The BB and RB1 bands are in turn separated by filter 87.

As with TPA section 12 and line site 40, amplifier 82 and 83 amplify the BB band and, respectively, the RB1 band, with a 980 nm pumping. To help stabilize the output power between channels in the RB1 band, amplifier 81 and 83 are preferably pumped with the same 980 nm laser diode pump source, by using a joining optical fiber 89 that transmits the residual 980 nm pump signal with relatively low loss. Specifically, amplifier 81 is associated with a WDM coupler, positioned between amplifier 81 and filter 87, that extracts the 980 nm pump light that remains at the output of amplifier 81. This WDM coupler may be, for example, model number SWDMCPR3PS110 supplied by E-TEK DYNAMICS, INC., 1885 Lundy Ave., San Jose, Calif. (USA). The output from this WDM coupler feeds into a second WDM coupler of the same type and positioned in the optical path after amplifier 83. The two couplers are joined by an optical fiber 89 that transmits the residual 980 nm pump signal with relatively low loss. The second WDM coupler passes the residual 980 nm pump power into amplifier 83 in a counter-propagating direction. Thus, amplifiers 81-83, filter 87 and equalizing filter 88 perform the same functions as amplifiers 64, 65 and 67, filter 71, and equalizing filter 74, respectively, of line site 40 and may comprise the same or equivalent parts depending on overall system requirements.

Amplifier 84 is coupled to filter 86 to receive and amplify the RB2 band. Amplifier 84 is, for example, an erbium-doped amplifier identical to the amplifier 68 of FIG. 6. RB2 band channels are then received by amplifier 85 that is, preferably, an erbium-doped amplifier of a known type.

RPA section 14 further comprises a routing stage 90, which permits to adapt the channel spacing within the BB, RB1 and RB2 bands to the channel separation capability of demultiplexing section 15. In particular, if the channel separation capability of demultiplexing section 15 is for a relatively wide channel spacing (e.g. 100 GHz grid) while channels in WDM system 1 are densely spaced (e.g. 50 GHz), then RPA section 14 could include the routing stage 90 shown in FIG. 7. Other structures may be added to RPA section 14 depending on the channel separation capability of demultiplexing section 15.

Routing stage 90 includes three router modules 91-93. Each router module 91-93 separates the respective band into two sub-bands, each sub-band including half of the channels of the corresponding band. For example, if the BB band includes sixteen (16) channels λ₁-λ₁₆, each separated by 50 GHz, then router module 91 would split the BB band into a first sub-band BB′ having channels λ₁, λ₃, . . . , λ₁₅ separated by 100 GHz and a second sub-band BB″ having channels λ₂, λ₄, . . . , λ₁₆ separated by 100 GHz and interleaved with the channels in the sub-band BB′. In a similar fashion, router modules 92 and 93 would split the RB1 band and the RB2 band, respectively, into first sub-bands RB1′ and RB2′ and second sub-bands RB1″ and RB2″.

Each router module 91-93 may, for example, include a coupler (not shown) that has a first series of Bragg gratings attached to a first port and a second series of gratings attached to a second port. The Bragg gratings attached to the first port would have reflection wavelengths that correspond to every other channel (i.e. the even channels), while the Bragg gratings attached to the second port would have reflection wavelengths that correspond to the remaining channels (i.e. the odd channels). This arrangement of gratings will also serve to split the single input path into two output paths with twice the channel-to-channel spacing.

After passing through RPA section 14, the BB, RB1 and RB2 bands or their respective sub-bands are received by demultiplexing section 15. As shown in FIG. 8, demultiplexing section 15 includes six wavelength demultiplexers (WDs) 95′, 95″, 96′, 96″, 97′, 97″ which receive the respective sub-bands BB′, BB″, RB1′, RB1″, RB2′ and RB2″ and generate the output channels 17. Demultiplexing section 15 further includes receiving units Rx1-Rx128 for receiving the output channels 17.

The wavelength demultiplexers preferably comprise arrayed waveguide grating devices, but alternate structures for achieving the same or similar wavelength separation are contemplated. For instance, one may use interferential filters, Fabry-Perot filters, or in-fiber Bragg gratings in a conventional manner to demultiplex the channels within the sub-bands BB′, BB″, RB1′, RB1″, RB2′, RB2″.

In a preferred configuration, demultiplexer section 15 combines interferential filter and AWG filter technology. Alternatively, one may use Fabry-Perot filters or in-fiber Bragg gratings. WDs 95′, 95″, which are preferably eight channel demultiplexers with interferential filters, receive and demultiplex first sub-band BB′ and second sub-band BB″, respectively. Specifically, WD 95′ demultiplexes channels λ₁, λ₃, . . . , λ₁₅, and WD 95″ demultiplexes channels λ₂, λ₄, . . . , λ₁₆ Both WD 95′ and WD 95″, however, may be 1×8 type AWG 100 GHz demultiplexers. Similarly, WDs 96′ and 96″ receive and demultiplex first sub-band RB1′ and second sub-band RB1″, respectively, to produce channels λ₁₇-λ₆₄ and WDs 97′ and 97″ receive and demultiplex first sub-band RB2′ and second sub-band RB2″, respectively, to produce channels λ₆₅-λ₁₂₈. Both WD 96′ and WD 96″ may be 1×32 type AWG 100 GHz demultiplexers that are underequipped to use only twenty-four of the available demultiplexer ports and both WD 97′ and WD 97″ may be 1×32 type AWG 100 GHz demultiplexers that uses all the available demultiplexer ports. Output channels 17 are composed of the individual channels demultiplexed by WDs 95′, 95″, 96′, 96″, 97′, 97″, and each channel of output channels 17 is received by one of receiving units Rx1×Rx128.

FIG. 9 illustrates an optical amplifier 100 according to the present invention. Optical amplifier 100 can be used in the optical transmission system 1, both in the amplifier section 53 of FIG. 4 and in the amplifier section 69 of FIG. 6, to amplify signals in the RB2 band.

Amplifier 100 is preferably a bidirectionally-pumped optical amplifier and includes:

an input port 101 for the input of optical signals to be amplified;

an output port 102 for the output of the optical signals after amplification;

an active fiber 103 having a first end 103 a optically coupled to the input port 101 and a second end 103 b optically coupled to the output port 102 and adapted to amplify the optical signals;

a first pump source 104 optically coupled to the active fiber 103 by means of a first optical coupler 105 and adapted to feed a first pump radiation to the active fiber 103, preferably in a co-propagating direction with respect to transmitted signals;

a second pump source 106 optically coupled to the active fiber 103 by means of a second optical coupler 107 and adapted to feed a second pump radiation to the active fiber 103, preferably in a counter-propagating direction with respect to transmitted signals.

Alternatively, by opportunely multiplexing the first pump radiation, the second pump radiation and the optical signal, the first pump radiation and the second pump radiation may be fed to the active fiber 103 in a same direction, preferably both in the co-propagating direction.

Alternatively, a plurality of pump sources may be used in place of the first pump source and/or the second pump source. This plurality of pump sources may be multiplexed either in wavelength (if operating at different wavelengths) or in polarization.

Amplifier 100 may also comprise a first optical isolator 108 of a known type positioned between input 101 and the first coupler 105, to allow light transmission only from input 101 to coupler 105, and/or a second optical isolator 109 of a known type positioned between the second coupler 107 and output 102, to allow light transmission only from the second coupler 107 to output 102.

Active fiber 103 is a silica fiber co-doped with erbium and ytterbium. Active fiber 103 is single-mode and has a length preferably comprised between 10 m and 30 m and a numeric aperture NA preferably comprised between 0.15 and 0.22. The core of active fiber 103 includes the following components with the indicated concentrations:

Al: between 0.1 and 13 atomic %;

P: between 0.1 and 30 atomic %;

Er: between 0.1 and 0.6 atomic %;

Yb: between 0.5 and 3.5 atomic %.

The ratio between erbium and ytterbium concentrations is preferably in the range between 1:5 and 1:30, for example 1:20.

The first coupler 105 is preferably a micro-optic interferential WDM coupler, including:

a first access fiber 105 a optically coupled to the input port 101 to receive the signals (in the RB2 band channels) to be amplified;

a second access fiber 105 b optically coupled to the first pump source 104 by means of a single-mode optical fiber 110, to receive the first pump radiation;

a third access fiber 105 c optically coupled to the active fiber 103 to feed to the active fiber 103 the optical signals to be amplified together (and in a same propagation direction) with the first pump radiation .

The first coupler 105 further includes a converging lens system (not shown), to opportunely direct the light beams among its access fibers, and a selective-reflection surface (not shown), e.g. a dichroic mirror. The actual inclination of the reflection surface inside the coupler depends on the direction of the incoming optical beams carrying the signal and the pump radiation. Preferably, the selective-reflection surface in coupler 105 is transparent for the wavelengths of the RB2 band channels and reflecting for the wavelength of the first pumping radiation. In this way, the RB2 band channels pass through the reflecting surface substantially without losses while the first pump radiation is reflected by the reflecting surface into the core of the active fiber 103. Alternatively, the first coupler 105 may include a selective-reflection surface that is reflecting for the wavelengths of the RB2 band channels and transmissive for the wavelength of the first pumping radiation.

The first coupler 105 has preferably an insertion loss for the optical signals not greater than 0.6 dB. For example, the first coupler 105 may be model MWDM-45/54 made by Oplink.

According to another embodiment, the first coupler 105 may be a fused-fiber like coupler.

The second coupler 107 is preferably a fused fiber WDM coupler including:

a first access fiber 107 a optically coupled to the output port 102 to feed to the output port 102 the amplified signals;

a second access fiber 107 b optically coupled to the second pump source 106 by means of an optical fiber 111, to receive the corresponding pump radiation;

a third access fiber 107 c optically coupled to the active fiber 103 to receive from the active fiber 103 the amplified optical signals and to feed to the active fiber 103 the pump radiation generated by the second pump source 106; and

a fourth access fiber 107 d having a free end, that is low-reflection terminated.

The second coupler 107 may be made by fusing a first fiber defining the first and the third access fiber 107 a, 107 c, and a second fiber defining the second and the fourth access fiber 107 b, 107 d.

The second coupler 107 has preferably an insertion loss for the optical signals not greater than 0.3 dB.

The first pump source 104 is preferably a semiconductor laser diode, providing the first pump radiation at a wavelength in the range between 1465 nm and 1495 nm, adapted to excite the Er ions in the active fiber 103. The pumping power provided by the first pump source 104 is preferably comprised between 40 mW and 150 mW. The first pump source 104 may be, for example, model number SLA5600-DA supplied by SUMITOMO ELECTRIC INDUSTRIES, Ltd.

Direct pumping of the Er ions, in particular co-directional pumping, is believed to originate a pre-amplification of the optical signals in the active fiber 103. This pre-amplification, in combination with a boosting effect provided by pumping the Yb ions, is believed to be the origin of the observed significant performance increase for the amplifier, in particular under low input power conditions.

The Applicant has found that pumping directly the Er ions in the 1480 nm band is preferable with respect to pumping in the 980 nm band. In fact, the 1480 nm pump radiation, differently from what would occur to a 980 nm pump radiation, is believed to be slowly absorbed in the active fiber so as to provide higher fluorescence at longer wavelengths (1600 nm). This allows the optical signal power to progressively rise along the active fiber avoiding an excessive ASE accumulation.

The proposed amplifier is able, as hereinbelow reported, to amplify optical signals with very low input powers, down to −25 dBm.

With reference to FIG. 10, the second pump source 106 preferably includes a fiber laser 112 and a pump laser diode 113. Advantageously, fiber laser 112 is adapted to generate the second pump radiation at a wavelength in the range between 1000 nm and 1100 nm, adapted to excite the Yb ions in the active fiber 103. Fiber laser 112 preferably comprises a double-cladding fiber 114 and a first and a second Bragg grating 118, 119. Bragg gratings 118, 119 are written into opposite ends of double-cladding fiber 114 and delimit the Fabry-Perot resonant cavity of the fiber laser 112.

Pump laser diode 113 is optically coupled to one end of the double-cladding fiber 114 and is adapted to generate an exciting radiation for pumping the double-cladding fiber 114. The opposite end of double-cladding fiber 114 is spliced to fiber 111 for transmitting the second pump radiation to active fiber 103.

FIG. 11a shows a not-in-scale cross section of double-cladding fiber 114. Fiber 114 includes a core 115 having a first refraction index n₁, an inner cladding 116 surrounding the core 115 and having a second refraction index n₂<n₁, and an outer cladding 117 surrounding the inner cladding 116 and having a third refraction index n₃ <n₂. Core 115, inner cladding 116 and outer cladding 117 are coaxial.

Fiber 114 is a silica fiber having the core 115 preferably doped with a high concentration of Yb, in order to generate the second pump radiation at a wavelength suitable for pumping the active fiber 103. Yb concentration in core 115 is preferably greater than 0.1 atomic %, more preferably comprised between 0.7 atomic % and 1.5 atomic %.

The concentrations of the other components of core 115 are preferably within the following ranges:

Ge: between 0.1 and 20 atomic %;

Al: between 0.1 and 6 atomic %;

P: between 0.1 and 20 atomic %.

Pump laser diode 113 is preferably a broad-area laser, with emission spectrum centered at a wavelength suitable to pump dopant ions in the double-cladding fiber 114, preferably comprised between 910 nm and 925 nm. Pump laser diode 113 is preferably provided with an output multi-mode optical fiber 120 having the core substantially of the same diameter and with the same numeric aperture of the inner cladding 116 of active fiber 114, in order to couple the excitation radiation into the active fiber 114 with a very high efficiency (near 100%).

As shown in FIG. 11b, under normal operating conditions, the pump radiation generated by the pump laser diode 113 is fed into the inner cladding 116 and is progressively absorbed by the core 115, exciting the Yb ions. The de-excitement of the Yb ions gives rise to stimulated emission in the wavelength range 1000-1100 nm, which propagates into the core 115 and amplifies itself. Gratings 118, 119 reflect a predetermined wavelength in the range 1000-1100 nm (for example 1047 nm), giving rise, after multiple reflections, to a high power laser radiation at this specific wavelength which is emitted from the end of fiber 114 opposite to the pump laser diode 113.

Fiber laser 112 may be realized by firstly producing the double-cladding fiber 114 with characteristics (length, geometry and composition) optimized according to the desired laser performances, and successively writing gratings 118 and 119 on the opposite ends of fiber 114.

To produce fiber 114, two different preforms (not shown) are used. A first preform is used to obtain the core 115 and an inner portion of the inner cladding 116. The first preform is made by deposing SiO₂, P₂O₅ and Al₂O₃ by means of the known “chemical vapor deposition” (CVD) method, and then by introducing the rare earth ytterbium by means of the known “solution doping” method. The first preform is then opportunely worked to reduce its external diameter to a predetermined value.

A second preform of a commercial-type is used to obtain an outer portion of the inner cladding 116 and the outer cladding 117. The second preform has a central region of pure SiO₂ and a surrounding region of fluoride-doped SiO₂. The central region of the second preform is partly removed so as to obtain a central longitudinal hole having a diameter slightly larger than the external diameter of the first preform, into which the first preform is introduced. The inner cladding is defined partly from the first preform and partly from the second preform.

The three-layer preform so obtained is drawn in the usual way to obtain the optical fiber 114.

Gratings 118 and 119 may be written by means of a grating writing assembly 130 shown in FIG. 12 and according to the technique hereinbelow described, developed by the Applicant.

With reference to FIG. 12, the grating writing assembly 130 the pump laser diode 113 optically coupled to a first end 114 a of fiber 114, an optical power measuring device 131, preferably a power meter, positioned in front of a second end 114 b of fiber 114 and, preferably, an optical band-pass filter 132 interposed between the second end 114 b of fiber 114 and the measuring device 131.

Measuring device 131 is, for example, a power meter of the type ANDO AQ2140.

Filter 132 is preferably an interferential filter, centered at the predetermined wavelength for the laser emission λ_(laser) of source 106.

Assembly 130 further includes a processor (PC) 134 adapted to control the pump laser diode 113 and the device 131 preferably by means of a DAC (Digital-Analog Converter) 133 and using a specific software (for example Labview®). DAC 133 may be for example of the type National Instruments PCI 6110E. As shown in FIG. 12, processor 134 is further adapted to provide (on a display) the P_(out)/P_(pump) characteristic of laser 106 during grating writing process, according to information provided by the measuring device 131.

Moreover, assembly 130 includes a UV writing device 135 suitable to write gratings 118, 119 on fiber 114. UV writing device 135 includes preferably an excimer laser equipment.

The method for writing the first grating 118 is herein described with reference to the flux diagram of FIG. 16 and to the schematic representation of FIG. 18a. The method includes the following steps:

defining a reflecting surface associated to the active fiber, preferably by cutting and cleaning (block 200) the second end 114 b of fiber 114 in order to reach a predetermined reflectivity R₂ at the interface glass/air, preferably of about 4%; this reflecting surface has a reflection wavelength band wider than the reflection wavelength band expected for the first grating;

feeding (block 210) pump radiation having an optical power Pi, to the active fiber 114 by means of the pump laser diode 113 in order to excite the dopant ions and to give rise to an amplified stimulated emission (ASE) defining a free-running emission;

writing (block 220), by means of UV writing device 105, the first grating 118 near the first end 114 a of fiber 114, with a spatial period corresponding to the predetermined laser wavelength λ_(laser); the first grating 118 has a varying reflectivity R₁ and defines, together with the second end 114 b of fiber 114, a resonant cavity allowing the stimulated emission to travel forward and backward in fiber 114 and to output as a laser emission at the wavelength λ_(laser);

scanning (block 230) repeatedly, during the writing step, the power of the pump radiation in a predetermined power range (possibly starting with zero power), by driving the pump laser diode 113 by means of processor 134 and DAC 133; the minimum value of the pump radiation power to have laser emission defines a threshold power P_(th) which depends on the grating intensity; the scanning period may be, for example, 15-20 s;

spectrally filtering (block 240) the optical radiation which is output from the second end 114 b of fiber 114, by means of filter 132; filtering allows to suppress residual pump radiation and, at the beginning of the writing process, the free running radiation;

measuring (block 250), during the writing and scanning steps, the optical power of the filtered output radiation, by means of the measuring device 131; measuring the optical power includes obtaining, during a scanning period, a predetermined number N (for example 10) of optical power values, each value being obtained by calculating the average value of the power detected in a predetermined measuring period (for example 2 s); the predetermined number N of optical power values and the predetermined measuring period being related to the value of the scanning period;

processing (block 260), preferably by performing a linear regression, the measured optical power in order to obtain the laser's efficiency η and threshold power P_(th); performing the linear regression comprises finding a straight line which defines a best-fitting of the N last points (corresponding to the N optical power values obtained during the last scanning period) on the P_(out)/P_(in) characteristic, and evaluating the slope and the intersection of the straight line with the P_(in) axis in order to obtain current values of η and P_(th);

checking (block 270) if the efficiency η is increasing, by comparing the current value of η (η_(curr), point A in FIG. 18a), i.e. the value of η related to the last scanning period, with the preceding value of η (η_(prec), point B in FIG. 18a), i.e. the value obtained in the preceding step of processing and related to the preceding scanning period; the current value η_(curr) of efficiency η is related to the current value of the first grating reflectivity R₁;

repeating, if the efficiency η is increasing (η_(curr)>η_(prec)), the steps of writing, scanning, filtering, monitoring, processing and checking (blocks 220-270);

stopping the process (block 280) when the laser's efficiency η begins to degrade, i.e. if the efficiency η is no more increasing (η_(curr)≦η_(prec)) having reached a limit value η_(limit) (point C in FIG. 18a); η_(limit) corresponds to a maximum value for the reflectivity R₁ of the first grating 108 (near 100%) and is the maximum efficiency obtainable with the considered value of R₂ (4%); if the writing process were continued over this point, η would decrease (point D in FIG. 18a) due to a grating degradation related to some incoming phenomena, like saturation of defect centers and reduction of interference fringe contrast;

evaluating (block 290), according to the efficiency limit value η_(limit), the final reflectivity of the first grating 118.

The described process for writing the first grating may have a total duration of a few minutes.

The first grating has preferably a reflection wavelength band between 0.3 nm and 1 nm, more preferably between 0.4 and 0.7 nm.

The reflecting surface used in the first step may alternatively be defined by a multi-layer interferential reflecting surface made on the second end 114 b, a separate portion of fiber including a grating, micro-optic elements like semi-reflecting mirrors or lens systems, or similars.

The Applicant has observed that the threshold power P_(th) is another parameter that can be used, for example in addition to the efficiency, to establish when the first grating writing must be stopped. In fact, the threshold power P_(th) decreases during the writing process and reaches a limit value P_(th,limit) when the efficiency reaches its limit value η_(limit). However, the Applicant has observed that the evaluation of P_(th) is more difficult than the evaluation of η and that the variations of P_(th) during the writing process are less than the variations of η. Moreover, the actual value of P_(th) is slightly different from the value obtainable from the linear regression. Therefore, the Applicant has observed that η is the preferred parameter to be used in the checking step.

Typically, the limit efficiency η_(limit) obtained at the end of the above process does not correspond to the maximum efficiency η_(max) obtainable for the fiber laser 112 (point E in FIG. 18a). In order to reach the maximum efficiency η_(max), it is typically necessary to write the second grating 119 and to optimize its reflectivity.

Writing only the first grating 118 may be sufficient in some applications in which the reflectivity of the second end of active fiber 114 allows to define a laser cavity with the desired characteristics. For example, the 4% reflectivity of the second end of active fiber 114 may be sufficient for a “in-air laser”, i.e. a laser whose output radiation is emitted directly in air.

For the considered use, the Applicant has observed that the presence of a second grating 119 having a reflectivity of at least 4% allows an improvement in the performance of the fiber laser 112.

The Applicant has further observed that the previously described writing technique is also suitable for writing the second grating 119, even if an additional attention must be paid to the second grating 119 actual spectral allocation. This is because the active fiber 114, during the writing step, changes its refraction index, and the grating wavelength peak then shifts. For remedying to this drawback, the second grating 119 is advantageously a relatively large band grating, so that the peak shifts are included in the grating's band. Preferably, the ratio between the reflecting band of the second grating and the reflecting band of the first grating is between 1,5 and 3. If the “phase mask” writing technique is used, a grating with an enlarged reflection band may be obtained by positioning, in front of the mask, a screen provided of a slit, which introduces a predetermined diffraction of the UV radiation.

Moreover, it is preferred to make an a priori evaluation of the possible peak shift during writing in order to reach an overlap of the peak related to the first grating 118 and the peak related to the second grating 119. This evaluation can be made by estimating the required duration of the writing process and the approximate shift per second of the grating peak.

The method for writing the second grating 119 is herein described with reference to the flux diagram of FIG. 17 and to the schematic representation of FIG. 18b. The method includes the following steps:

cutting (block 300) the second end 114 b of active fiber 114 to obtain and end surface inclined with an angle of 7-8° (with respect to a plane perpendicular to the fiber axis) having a negligible reflectivity;

feeding (block 310) pump radiation having an optical power P_(in) to the active fiber 114 by means of the pump laser diode 113 in order to excite the dopant ions of the active fiber 114;

writing (block 320), by means of UV writing device 105, the second grating 119 near the second end 114 b of fiber 114, with a spatial period corresponding to the predetermined laser wavelength λ_(laser); the second grating 119 has a varying reflectivity R₂ and defines, together with the first grating 118 which has a reflectivity R₁ near 100%, a resonant cavity allowing the stimulated emission to travel forward and backward in fiber 114 and to output as a laser emission at the wavelength λ_(laser);

scanning (block 330) repeatedly, during the writing step, the power of the pump radiation in a predetermined power range (which may be different from the range used for the first grating writing), by driving the pump laser diode 113 by means of processor 134 and DAC 133; the minimum value of the pump radiation power to have laser emission defines a threshold power P_(th) which depends on the second grating intensity;

spectrally filtering (block 340) the optical radiation which is output from the second end 114 b of fiber 114, by means of filter 132; filtering allows to suppress residual pump radiation and, at the beginning of the second grating writing, the possible free running radiation;

measuring (block 350), during the writing and scanning steps, the optical power of the filtered output radiation, by means of the measuring device 131; measuring the optical power includes obtaining, during a scanning period, a predetermined number N′ (which may be different from the predetermined number N used for the first grating writing) of optical power values, each value being obtained by calculating the average value of the power detected in a predetermined measuring period; the predetermined number N′ of optical power values and the predetermined measuring period being related to the duration of the scanning period;

processing (block 360), preferably by performing a linear regression, the measured optical power in order to obtain the laser's efficiency η and threshold power P_(th); performing the linear regression comprises finding a straight line which defines a best-fitting of the N′ last points (corresponding to the N′ optical power values obtained during the last scanning period) on the P_(out)/P_(in) characteristic, and evaluating the slope and the intersection of the straight line with the P_(in) axis in order to obtain current values of η and P_(th); the first detected value of η will be intermediate between zero and the limit value η_(limit) found at the end of the first grating writing;

checking (block 370) if the efficiency η is increasing, by comparing the current value of η (η_(curr), point A in FIG. 18b), i.e. the value of η related to the last scanning period, with the preceding value of η (η_(prec), point B in FIG. 18b), i.e. the value obtained in the preceding step of processing and related to the preceding scanning period; the current value η_(curr) of efficiency η is related to the current value of the second grating reflectivity R₂;

repeating, if the efficiency η is increasing (η_(curr)>η_(prec)) the steps of writing, scanning, filtering, monitoring, processing and checking (blocks 320-370);

stopping the process (block 380) when the lasers efficiency η begin to degrade, i.e. if the efficiency η is no more increasing (η_(curr)<η_(prec)) having reached a maximum value η_(max) (point E in FIG. 18b); η_(max) corresponds to an optimum value R_(2,opt) for the reflectivity R₂ of the second grating 109 (for example included between 4 and 10%) and represents the maximum efficiency obtainable for the fiber laser 112; if the writing process were continued over this point, η would decrease (point D in FIG. 18b) due to a grating degradation related to some incoming phenomena, like saturation of defect centers and reduction of interference fringe contrast;

evaluating (block 390), according to the maximum value of efficiency η_(max), the final reflectivity of the second grating 119.

The Applicant has observed that, during the second grating writing process (R₂ increasing), the threshold power P_(th) progressive decreases and this trend continues over the optimum value R_(2,opt). Having a lower value of the threshold power P_(th) is an advantage in that it allows lasering with a lower input power. Thus, a further improved criterion to optimize the fiber laser 112 performances would be that of stopping the process when the best compromise, or a predetermined relation, between the efficiency η and the threshold power P_(th) has been reached.

This compromise may depend on the particular application considered.

Experimental Results on Amplifying Unit 100 Performances

Experimental measurements have been carried out on an amplifying unit 100 whose characteristics are hereinbelow described in detail.

An active fiber 103 used in the experiment has a core diameter of 4.3 μm, a cladding diameter of 125 μm, a numeric aperture NA=0.2 and is composed as follows:

element Si Al P Er Yb atomic % 70.8 1.5 25 0.125 2.5

The ratio of Er and Yb concentrations is about 1:20.

The first coupler 105 is an interferential filter model MWDM-45/54 made by OPLINK. The first coupler 105 has an insertion loss of 0.6 dB.

The second coupler 107 is a fused fiber WDM coupler. The second coupler 107 is, according to the above, made by fusing a first fiber defining access fibers 107 a and 107 c and a second fiber defining access fibers 107 b and 107 d. The first fiber is a SM (single-mode) fiber having a core diameter of 3.6 μm, a cladding diameter of 125 μm and a numeric aperture NA=0.195. The second fiber is a SM fiber having a core diameter of 3.6 μm, a cladding diameter of 125 μm and a numeric aperture NA=0.195. Both SM fibers are of the type CS 980 produced by Corning. The second coupler 107 has an insertion loss of 1 dB.

The first pump source 104 is a laser diode adapted to provide a pump radiation power of 50-70 mW at 1480 nm. Fiber 110 is a SM fiber.

The second pump source 106 has been made by the Applicant and is adapted to provide a pump radiation power of 500-650 mW at 1047 nm. Fiber 111 is a SM fiber. Broad area diode laser 113 is adapted to provide a radiation power of 800 mW at 915 nm. The Applicant observes that a much higher saturation power of the amplifier could probably be obtained by using a more powerful broad area diode laser.

Active fiber 114 in the second pump source has, in its core 115, the following composition, detected by means of a SEM analysis.

element Si Ge Al P Yb atomic % 89.40 2.78 1.17 5.93 0.72

Al concentration has been chosen relatively high in order to obtain a high concentration of Yb. Ge concentration is relatively low, due to the high value of the refraction index determined by the high concentration of Al and Yb. P has been added in order to reduce the numeric aperture (NA) of the fiber.

The length of active fiber 114 is 10 m and its bending diameter is about 40 mm. The Applicant has observed that this value of the bending diameter represent the best compromise between absorbing efficiency and induced losses in the fiber.

The length of the resonant cavity (i.e. the distance between the first and the second grating 118, 119) is approximately 10 m.

The active fiber 114 has an external diameter of the outer cladding 117 of about 90 μm, an external diameter of the inner cladding 116 of about 45 μm and an external diameter of the core 115 of about 4.5 μm. The refraction index step Δn=n₁-n₂ between the core 115 and the inner cladding 116 is about 0.0083 and the refraction index step Δn′=n₂-n₃ between the inner cladding 116 and the outer cladding 117 is about 0.067. The core 115 and the inner cladding 116 define a single-mode waveguide for the conveying of transmission signals, having a first numeric aperture NA₁ of about 0.155, while the inner cladding 116 and the outer cladding 117 define a multi-mode waveguide for the conveying of pump radiation, having a second numeric aperture NA₂ of about 0.22.

Gratings 118, 119 have been realized by the method previously described. Gratings 118, 119 have a Bragg wavelength of 1047 nm. The first grating 118 has a reflectivity of about 99% at peak wavelength and the second grating 119 has a reflectivity less then 10% at the same wavelength.

FIG. 13 shows the response curve of fiber laser 112. In particular, FIG. 13 shows the dependence of the optical power P_(out) of the emitted laser radiation on the pump power P_(in) provided by laser diode 113. According to the obtained curve, the laser source has an efficiency η=81,5% and a threshold power P_(th)=99 mW.

FIG. 14 shows the insertion losses due to the passive components of the amplifier 100 placed, respectively, between the input 101 and the first end of the fiber 103 (i.e. the first optical isolator 108 and the first optical coupler 105), and between the second end of the fiber 103 and the output 102 (i.e. the second optical coupler 107 and the second optical isolator 109). The characteristics of FIG. 14 have been obtained by means of an optical spectrum analyzer.

FIG. 15 shows the gain curves of the amplifying unit 100, for a wavelength scanning of the input signal from 1575 nm to 1620 nm. The different curves in FIG. 15 refer to input signal powers within the range −25 dBm and 10 dBm. It can be noticed that, for input signal power greater than 0 dBm, the amplifying unit 100 provides output power greater than about 18 dBm and can then be used as a booster amplifier. In particular, at 10 dBm of input signal power, the unit provides up to 22 dBm output power with a maximum gain variation less than 1 dB in the RB2 band.

When amplifier 100 is used as a booster unit, with an input signal of 10 dBm or more, the gain curve exhibits a maximum variation less than 1 dB in the RB2 band.

Moreover, the amplifier 100 exhibits a gain extended beyond the RB2 band, as far as 1620 nm.

Numerical Results of Grating Writing Method Simulation

FIGS. 19-21 illustrates numerical results obtained by simulating the above described grating writing method on an active fiber 114 having the characteristics hereinabove listed in the experimental measurement.

FIG. 19 shows the dependence of optical output power P_(out) on the pump optical power P_(in) for different values of the first grating reflectivity during the first grating writing process. The resonant cavity is defined by the first grating 118 and the second end 114 b (4% reflectivity) of fiber 114. It can be observed the progressive increase of the fiber laser efficiency and the progressive decrease of the threshold power P_(th) with the increase of the first grating reflectivity.

FIG. 20 shows the dependence of efficiency η and threshold power P_(th) of fiber laser 112 on the first grating reflectivity during the first grating writing process. Each point on the η and P_(th) characteristics corresponds to a straight line of FIG. 19.

FIG. 21 shows the dependence of efficiency η and threshold power P_(th) of fiber laser 112 on the second grating reflectivity during the second grating writing process, in the assumption of a first grating reflectivity of 99%. A maximum in the efficiency curve is detectable for a second grating reflectivity of about 4%, having a value greater than 80%. If the best compromise (between η and P_(th),) criterion is used, the writing process should advantageously be stopped when the second grating reflectivity is between 4% and 10%. 

What is claimed is:
 1. Method for writing grating for a fiber laser, the method comprising the following steps: providing a length of optically active fiber having a rare-earth-doped core photosensitized in a first region and a second region for defining the length of the optically active fiber having a reflecting surface in the second region and having the first region for preparing a first grating, said reflecting surface having a second reflection wavelength band wider than a first reflection wavelength band expected for the first grating; controlling a power level of pump radiation power by scanning the power of the pump radiation in a predetermined power range by a processor; optically pumping the length of the optically active fiber at the power level scanned to excite the rare-earth-doped core to provide an amplified stimulated emission through the first or second region as a free-running emission; writing the first grating in the first region, in order to allow the amplified stimulated emission to travel forward and backward between the first grating and the reflecting surface and to consequently induce a laser emission from the optically active fiber by captivating the free-running emission; measuring, during the step of writing the first grating, the optical power of the laser emission at the power level scanned; determining by the processor a ratio of the optical power of the laser emission divided by the power level scanned in order to obtain a current value of the laser efficiency; comparing the current value of the laser efficiency at a current scan increment to a preceding value of the laser efficiency at a previous scan increment; returning to the power level step to increase the power level of pump radiation power by a new current scan increment when the current value is less than the preceding value of the laser efficiency; controlling by the processor the step of writing the first grating according to the measured optical power such that when the current value is greater than the preceding value of the laser efficiency for reaching a limit value, stopping the step of writing the first grating.
 2. Method according to claim 1, characterized in that it includes writing in the optically active fiber, subsequently to the first grating, a second grating in the second region for providing the reflecting surface, the second grating suitable to define, together with the first grating, a resonant cavity for said fiber laser.
 3. Method according to claim 2, characterized in that it includes the following steps: optically pumping the active fiber, during the step of writing the second grating, in order to excite an amplified stimulated emission between said first and second gratings and consequently induce a laser emission from the active fiber; measuring, during the step of writing the second grating, the optical power of the laser emission; controlling by the processor the step of writing the second grating according to the comparison of current to previous laser efficiency values.
 4. Method according to claim 3, characterized in that it includes, during the step of writing the second grating, scanning the power of the pump radiation in a predetermined power range.
 5. Method according to claim 4, characterized in that the step of scanning is repeated with a predetermined scanning period and the step of measuring the optical power includes obtaining a predetermined number of optical power values during the predetermined scanning period.
 6. Method according to claim 5, characterized in that the step of obtaining a predetermined number of optical power values includes calculating by the processor, to obtain each of said optical power values, the average value of the optical power measured in a predetermined measuring period.
 7. Method according to claim 5, characterized in that it includes the step of processing by the processor said optical power values in order to obtain a current value of the laser efficiency.
 8. Method according to claim 7, characterized in that the step of processing comprises obtaining by the processor from said optical power values a current value of the laser threshold power.
 9. Method according to claim 8, characterized in that the step of controlling the step of writing includes stopping by the processor the step of writing the second grating when a predetermined relation between said current values of the laser efficiency and the threshold power has been reached.
 10. Method according to claim 7, characterized in that the step of controlling the step of writing includes checking by the processor if said current value of the laser efficiency has reached a maximum value and, if said maximum value has been reached, stopping the step of writing the second grating.
 11. Method according to claim 10, characterized in that it further includes evaluating by the processor, according to said maximum value, the reflectivity of said second grating.
 12. Method according to claim 2, characterized in that it includes, before the step of writing the second grating, providing a zone of negligible reflectivity in place of said reflecting surface.
 13. Method according to claim 2, characterized in that the second grating has a third reflection wavelength band and the ratio between the third and the first reflection wavelength bands is between 1.5 and
 3. 14. Method according to claim 1, characterized in that it includes, during the step of writing the first grating, monitoring the power of the pump radiation in the predetermined power range.
 15. Method according to claim 14, characterized in that the step of monitoring is repeated with a predetermined scanning period for providing the scan increment and the step of measuring the optical power includes obtaining a predetermined number of optical power values during the predetermined scanning period.
 16. Method according to claim 15, characterized in that the step of obtaining a predetermined number of optical power values includes calculating by the processor, to obtain each of said optical power values, the average value of the optical power measured in a predetermined measuring period.
 17. Method according to claim 15, characterized in that it includes the step of processing by the processor said optical power values in order to obtain a current value of the laser efficiency.
 18. Method according to claim 17, characterized in that the step of processing comprises finding a fitting line for a predetermined number of points on a laser gain characteristic corresponding to said optical power values, and evaluating the slope of said line by the processor.
 19. Method according to claim 17, characterized in that the step of controlling the step of writing includes checking if said current value of the laser efficiency has reached the limit value and, if said limit value has been reached, stopping the step of writing the first grating.
 20. Method according to claim 19, characterized in that the step of checking includes comparing by the processor said current value of the laser efficiency, related to a last scanning period, with a preceding value of the laser efficiency related to a preceding scanning period.
 21. Method according to claim 19, characterized in that it further includes evaluating by the processor, according to said limit value, the reflectivity of said first grating.
 22. Method according to claim 1, characterized in that the step of providing the length of optically active fiber having the reflecting surface includes cutting and cleaning one end of the optically active fiber in order to define the reflecting surface at the interface glass/air.
 23. Method according to claim 1, characterized in that the active fiber includes an active fiber having an absorption of at least 15 dB in a range of about ±10 nm centered at a wavelength corresponding to a maximum reflection wavelength of said first grating.
 24. Method according to claim 1, characterized in that the active fiber includes a double-cladding active fiber. 